{"id":4520,"date":"2022-05-04T10:01:18","date_gmt":"2022-05-04T08:01:18","guid":{"rendered":"https:\/\/www.dm.unipi.it\/eventi\/non-homogeneous-persistent-random-walks-and-averaged-environment-for-the-levy-lorentz-gas-giampaolo-cristadoro-universita-di-milano-bicocca\/"},"modified":"2022-05-04T10:01:18","modified_gmt":"2022-05-04T08:01:18","slug":"non-homogeneous-persistent-random-walks-and-averaged-environment-for-the-levy-lorentz-gas-giampaolo-cristadoro-universita-di-milano-bicocca","status":"publish","type":"unipievents","link":"https:\/\/www.dm.unipi.it\/en\/eventi\/non-homogeneous-persistent-random-walks-and-averaged-environment-for-the-levy-lorentz-gas-giampaolo-cristadoro-universita-di-milano-bicocca\/","title":{"rendered":"Non-homogeneous persistent random walks and averaged environment for the L\u00e9vy-Lorentz gas &#8211; Giampaolo Cristadoro (Universit\u00e0 di Milano-Bicocca)"},"content":{"rendered":"<h4>Venue<\/h4>\n<p>Sala Riunioni (Dip. Matematica).<\/p>\n<h4 class='mt-4'>Abstract<\/h4>\n<p>I will first introduce a model known in the physical literature as the L\u00e9vy-Lorentz gas. The model describes the continuous-time motion of a particle on the real line in the presence of a random array of marked points, whose nearest-neighbor distances are i.i.d. and long-tailed (with finite mean but possibly infinite variance, with controlling parameter $\\alpha$). I will give a brief summary of the know results about transport properties for this model. I will then present a related modelthat may be viewed as a mean-field version of the L\u00e9vy-Lorentz gas. This will naturally lead toconsider transport properties for a non-homogeneous persistent random walk.Depending on the values of $\\alpha$, the model shows a transition from normal transport to superdiffusion, which is characterized by appropriate continuum limits. Joint work with Roberto Artuso, Mattia Radice and Manuele Onofri <\/p>\n","protected":false},"excerpt":{"rendered":"<p>I will first introduce a model known in the physical literature as the L\u00e9vy-Lorentz gas. The model describes the continuous-time motion of a particle on the real line in the presence of a random array of marked points, whose nearest-neighbor&hellip;<\/p>\n<p><a class=\"btn btn-dark btn-sm unipi-read-more-link\" href=\"https:\/\/www.dm.unipi.it\/en\/eventi\/non-homogeneous-persistent-random-walks-and-averaged-environment-for-the-levy-lorentz-gas-giampaolo-cristadoro-universita-di-milano-bicocca\/\">Read More&#8230;<\/a><\/p>\n","protected":false},"author":6,"featured_media":0,"template":"","tags":[],"unipievents_taxonomy":[],"class_list":["post-4520","unipievents","type-unipievents","status-publish","hentry"],"acf":[],"unipievents_startdate":1530723600,"unipievents_enddate":1530727200,"unipievents_place":"Sala Riunioni (Dip. Matematica).","unipievents_externalid":0,"jetpack_sharing_enabled":true,"publishpress_future_workflow_manual_trigger":{"enabledWorkflows":[]},"_links":{"self":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents\/4520","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents"}],"about":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/types\/unipievents"}],"author":[{"embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/users\/6"}],"version-history":[{"count":0,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents\/4520\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/media?parent=4520"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/tags?post=4520"},{"taxonomy":"unipievents_taxonomy","embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents_taxonomy?post=4520"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}